Low-energy description of the metal-insulator transition in the rare-earth nickelates
arXiv:1410.2830 · doi:10.1103/PhysRevB.91.075128
Abstract
We propose a simple theoretical description of the metal-insulator transition of rare-earth nickelates. The theory involves only two orbitals per nickel site, corresponding to the low-energy anti-bonding states. In the monoclinic insulating state, bond-length disproportionation splits the manifold of bands, corresponding to a modulation of the effective on-site energy. We show that, when subject to a local Coulomb repulsion and Hund's coupling , the resulting bond-disproportionated state is a paramagnetic insulator for a wide range of interaction parameters. Furthermore, we find that when is small or negative, a spontaneous instability to bond disproportionation takes place for large enough . This minimal theory emphasizes that a small or negative charge-transfer energy, a large Hund's coupling, and a strong coupling to bond-disproportionation are the key factors underlying the transition. Experimental consequences of this theoretical picture are discussed.
17 pages, 10 figures; published version in the update
References in corpus (4)
- Continuous-time Monte Carlo methods for quantum impurity models
- Strong electronic correlations from Hund's coupling
- Plane-wave based electronic structure calculations for correlated materials using dynamical mean-field theory and projected local orbitals
- Hund's coupling key role in multi-orbital correlations
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